Still, for a full solution to the HP, taming or even cutting completely off the top-loop contribution is not enough and around \(\Lambda _{\rm NP}=10\)  TeV, at the latest, a full UV completion – taking care of contributions from bosonic loops – should kick in.Note that our mechanism becomes even more effective for scenarios where the NP couples mostly through the top sector, leading to further increased cutoff. Moreover, it could also address other new interactions, potentially breaking the Higgs shift symmetry in an energy-scale dependent way.
The scenario discussed here would thus play an assistant role, relieving the strong bound from the top partner searches, when being combined with traditional solutions like SUSY and CHM. It is especially helpful in composite theories, where an \(\mathcal {O}(1)\)  Yukawa coupling (breaking explicitly the Goldstone symmetry) is problematic. In fact, this large value is the main reason for the currently biggest tension of such models with
LHC data, which is the absence of expected light top partners [1]}, [2]}, [3]}, [4]}, [5]}, [6]}, [7]} (see also [8]}, [9]}).
